By Vo Hoang Duy, Tran Trong Dao, Sang Bong Kim, Nguyen Tan Tien, Ivan Zelinka
This publication gathers the court cases of the foreign convention on complicated Engineering – thought and purposes (AETA 2016), held in Busan, Korea, from December eight to ten, 2016. It provides a variety of state of the art contributions from interrelated fields like electric engineering, keep an eye on engineering, energy electronics and distribution, telecommunication units, and so on. the most themes coated are: strength (energy-saving strength electronics, electric machines and force platforms, green-energy IT, nontrivial dynamics of digital devices), keep an eye on Engineering (robotics, automated keep an eye on, bio-sensor IT), and communique and protection (broadcasting IT, communications, cyber security).
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Extra info for AETA 2016: Recent Advances in Electrical Engineering and Related Sciences: Theory and Application
2 mm from the clamped position (note that the diameter of a tool is 10 mm). In the wall region, prediction of a thickness is a good agreement with the sine law. 35 mm. There is a good agreement between simulation results and measured values. It is worth to mention that the thickness of real part varies slightly, because of small tool radius and large step size. Fig. 4. Thickness distribution in different distant 6 Conclusion This paper presented a numerical procedure to implement the modiﬁed VBO model into FEM environment for simulating the ISF process with PP sheet.
Lee et al. state. In the analysis, the operating pressure and the design pressure were applied to the inner surfaces shown in Fig. 3 to investigate the changes in the contact pressure and stress levels. 17 MPa, respectively. Five load steps are used in the analysis, in which step 3 and step 5 are the steps to apply the operating pressure and the design pressure respectively while step 1 is the step to tighten the bolts. The contact occurs not only in the surfaces of the gasket in contact with the flange grooves but in the surfaces of bolts and nuts contacted with the outer surfaces of two flanges.
The evolution equation for the equilibrium stress G has two hardening terms followed by the modiﬁed dynamic recovery term and ﬁnally a term multiplied by the time rate of the kinematic stress f The growth law for the equilibrium stress is homogeneous of ﬁrst order in the rates and given by: ! w r À G ðG À f Þ r À G w _ r_ G_ ¼ w þ þ 1 À À f ð2Þ k kA þ bC k E E E W is the shape function which serves to control the transition between the initial quasi-elastic and region of plastic flow.